Different entropy-like quantities in nuclear physics have been considered
in [1]}, [2]}.
It has been found that “the thermodynamic entropy \(\ldots \) , the information
entropy \(\ldots \)  and the single-particle entropy \(\ldots \) , all
coincide for strong enough interaction but only in the presence
of a mean field” [2]}.
It is not possible to accept interpretation of these results in
Ref. [4]} as that \(S_{\rm th}\)  and \(S_{\rm sp}\)  “are nearly the
same only for noninteracting particles”.
Notice, correspondence between \(S_{\rm th}\)  and \(S_{\rm sp}\)  in a mean field
plus residual forces (Figs. 56(IIa, IIc) in [1]}) is
definitely not worse than in an almost pure mean field approach
(Figs. 56(Ia, Ic) in [1]}) .
